© 2005 Paul Dawkins
Trig Cheat Sheet
Definition of the Trig Functions Right triangle definition For this definition we assume that
02p
q< < or 0 90q° < < ° .
oppositesin
hypotenuseq = hypotenusecsc
oppositeq =
adjacentcoshypotenuse
q = hypotenusesecadjacent
q =
oppositetanadjacent
q = adjacentcotopposite
q =
Unit circle definition For this definition q is any angle.
sin
1y yq = = 1csc
yq =
cos1x xq = = 1sec
xq =
tan yx
q = cot xy
q =
Facts and Properties Domain The domain is all the values of q that can be plugged into the function. sinq , q can be any angle cosq , q can be any angle
tanq , 1 , 0, 1, 2,2
n nq pÊ ˆπ + = ± ±Á ˜Ë ¯
…
cscq , , 0, 1, 2,n nq pπ = ± ± …
secq , 1 , 0, 1, 2,2
n nq pÊ ˆπ + = ± ±Á ˜Ë ¯
…
cotq , , 0, 1, 2,n nq pπ = ± ± … Range The range is all possible values to get out of the function.
1 sin 1q- £ £ csc 1 and csc 1q q≥ £ - 1 cos 1q- £ £ sec 1 andsec 1q q≥ £ -
tanq-• < < • cotq-• < < •
Period The period of a function is the number, T, such that ( ) ( )f T fq q+ = . So, if w is a fixed number and q is any angle we have the following periods.
( )sin wq Æ 2T pw
=
( )cos wq Æ 2T pw
=
( )tan wq Æ T pw
=
( )csc wq Æ 2T pw
=
( )sec wq Æ 2T pw
=
( )cot wq Æ T pw
=
q adjacent
opposite hypotenuse
x
y
( ),x y
q
x
y 1
© 2005 Paul Dawkins
Formulas and Identities Tangent and Cotangent Identities
sin costan cotcos sin
q qq q
q q= =
Reciprocal Identities 1 1csc sin
sin csc1 1sec cos
cos sec1 1cot tan
tan cot
q qq q
q qq q
q qq q
= =
= =
= =
Pythagorean Identities 2 2
2 2
2 2
sin cos 1tan 1 sec1 cot csc
q q
q q
q q
+ =
+ =
+ =
Even/Odd Formulas ( ) ( )( ) ( )( ) ( )
sin sin csc csc
cos cos sec sec
tan tan cot cot
q q q q
q q q q
q q q q
- = - - = -
- = - =
- = - - = -
Periodic Formulas If n is an integer.
( ) ( )( ) ( )( ) ( )
sin 2 sin csc 2 csc
cos 2 cos sec 2 sec
tan tan cot cot
n n
n n
n n
q p q q p q
q p q q p q
q p q q p q
+ = + =
+ = + =
+ = + =Double Angle Formulas
( )( )
( )
2 2
2
2
2
sin 2 2sin cos
cos 2 cos sin
2cos 11 2sin
2 tantan 21 tan
q q q
q q q
q
=
= -
= -
= -
=-
Degrees to Radians Formulas If x is an angle in degrees and t is an angle in radians then
180and 180 180
t x tt xx
p pp
= fi = =
Half Angle Formulas
( )( )
( )( )( )( )
2
2
2
1sin 1 cos 221cos 1 cos 221 cos 2
tan1 cos 2
q q
q q
q
= -
= +
-=
+
Sum and Difference Formulas ( )( )
( )
sin sin cos cos sin
cos cos cos sin sintan tantan
1 tan tan
a b a b a b
a b a b a b
a ba b
a b
± = ±
± =
±± =
m
m
Product to Sum Formulas
( ) ( )
( ) ( )
( ) ( )
( ) ( )
1sin sin cos cos21cos cos cos cos21sin cos sin sin21cos sin sin sin2
a b a b a b
a b a b a b
a b a b a b
a b a b a b
= - - +È ˘Î ˚
= - + +È ˘Î ˚
= + + -È ˘Î ˚
= + - -È ˘Î ˚
Sum to Product Formulas
sin sin 2sin cos2 2
sin sin 2cos sin2 2
cos cos 2cos cos2 2
cos cos 2sin sin2 2
a b a ba b
a b a ba b
a b a ba b
a b a ba b
+ -Ê ˆ Ê ˆ+ = Á ˜ Á ˜Ë ¯ Ë ¯
+ -Ê ˆ Ê ˆ- = Á ˜ Á ˜Ë ¯ Ë ¯
+ -Ê ˆ Ê ˆ+ = Á ˜ Á ˜Ë ¯ Ë ¯
+ -Ê ˆ Ê ˆ- = - Á ˜ Á ˜Ë ¯ Ë ¯
Cofunction Formulas
sin cos cos sin2 2
csc sec sec csc2 2
tan cot cot tan2 2
p pq q q q
p pq q q q
p pq q q q
Ê ˆ Ê ˆ- = - =Á ˜ Á ˜Ë ¯ Ë ¯Ê ˆ Ê ˆ- = - =Á ˜ Á ˜Ë ¯ Ë ¯Ê ˆ Ê ˆ- = - =Á ˜ Á ˜Ë ¯ Ë ¯
© 2005 Paul Dawkins
Unit Circle
For any ordered pair on the unit circle ( ),x y : cos xq = and sin yq = Example
5 1 5 3cos sin3 2 3 2p pÊ ˆ Ê ˆ= = -Á ˜ Á ˜
Ë ¯ Ë ¯
3p
4p
6p
2 2,2 2
Ê ˆÁ ˜Á ˜Ë ¯
3 1,2 2
Ê ˆÁ ˜Á ˜Ë ¯
1 3,2 2
Ê ˆÁ ˜Á ˜Ë ¯
60°
45°
30°
23p
34p
56p
76p
54p
43p
116p
74p
53p
2p
p
32p
0 2p
1 3,2 2
Ê ˆ-Á ˜
Ë ¯
2 2,2 2
Ê ˆ-Á ˜
Ë ¯
3 1,2 2
Ê ˆ-Á ˜
Ë ¯
3 1,2 2
Ê ˆ- -Á ˜
Ë ¯
2 2,2 2
Ê ˆ- -Á ˜
Ë ¯
1 3,2 2
Ê ˆ- -Á ˜
Ë ¯
3 1,2 2
Ê ˆ-Á ˜
Ë ¯
2 2,2 2
Ê ˆ-Á ˜
Ë ¯
1 3,2 2
Ê ˆ-Á ˜
Ë ¯
( )0,1
( )0, 1-
( )1,0-
90° 120°
135°
150°
180°
210°
225°
240° 270°
300° 315°
330°
360°
0° x
( )1,0
y
© 2005 Paul Dawkins
Inverse Trig Functions Definition
1
1
1
sin is equivalent to sincos is equivalent to costan is equivalent to tan
y x x yy x x yy x x y
-
-
-
= =
= =
= =
Domain and Range
Function Domain Range 1siny x-= 1 1x- £ £
2 2yp p
- £ £
1cosy x-= 1 1x- £ £ 0 y p£ £
1tany x-= x-• < < • 2 2
yp p- < <
Inverse Properties ( )( ) ( )( )( )( ) ( )( )( )( ) ( )( )
1 1
1 1
1 1
cos cos cos cos
sin sin sin sin
tan tan tan tan
x x
x x
x x
q q
q q
q q
- -
- -
- -
= =
= =
= =
Alternate Notation
1
1
1
sin arcsincos arccostan arctan
x xx xx x
-
-
-
=
=
=
Law of Sines, Cosines and Tangents
Law of Sines sin sin sin
a b ca b g
= =
Law of Cosines 2 2 2
2 2 2
2 2 2
2 cos2 cos2 cos
a b c bcb a c acc a b ab
a
b
g
= + -
= + -
= + -
Mollweide’s Formula ( )1
212
cossin
a bc
a bg-+
=
Law of Tangents ( )( )( )( )( )( )
1212
1212
1212
tantan
tantan
tantan
a ba b
b cb c
a ca c
a ba b
b gb g
a ga g
--=
+ +
--=
+ +
--=
+ +
c a
b
a
b
g
Common Derivatives and Integrals
Visit http://tutorial.math.lamar.edu for a complete set of Calculus I & II notes. © 2005 Paul Dawkins
Derivatives Basic Properties/Formulas/Rules
( )( ) ( )dcf x cf x
dx
¢= , c is any constant. ( ) ( )( ) ( ) ( )f x g x f x g x¢ ¢ ¢± = ±
( ) 1n ndx nx
dx
-= , n is any number. ( ) 0dc
dx= , c is any constant.
( )f g f g f g¢ ¢ ¢= + – (Product Rule) 2
f f g f g
g g
¢ ¢ ¢Ê ˆ -=Á ˜
Ë ¯ – (Quotient Rule)
( )( )( ) ( )( ) ( )df g x f g x g x
dx
¢ ¢= (Chain Rule)
( )( ) ( ) ( )g x g xdg x
dx
¢=e e ( )( ) ( )( )
lng xd
g xdx g x
¢=
Common Derivatives Polynomials
( ) 0dc
dx= ( ) 1d
xdx
= ( )dcx c
dx= ( ) 1n nd
x nxdx
-= ( ) 1n ndcx ncx
dx
-=
Trig Functions
( )sin cosdx x
dx= ( )cos sind
x xdx
= - ( ) 2tan secdx x
dx=
( )sec sec tandx x x
dx= ( )csc csc cotd
x x xdx
= - ( ) 2cot cscdx x
dx= -
Inverse Trig Functions
( )1
2
1sin1
dx
dx x
- =-
( )1
2
1cos1
dx
dx x
- = --
( )12
1tan1
dx
dx x
- =+
( )1
2
1sec1
dx
dx x x
- =-
( )1
2
1csc1
dx
dx x x
- = --
( )12
1cot1
dx
dx x
- = -+
Exponential/Logarithm Functions
( ) ( )lnx xda a a
dx= ( )x xd
dx=e e
( )( ) 1ln , 0dx x
dx x= > ( ) 1ln , 0d
x xdx x
= ≠ ( )( ) 1log , 0lna
dx x
dx x a= >
Hyperbolic Trig Functions
( )sinh coshdx x
dx= ( )cosh sinhd
x xdx
= ( ) 2tanh sechdx x
dx=
( )sech sech tanhdx x x
dx= - ( )csch csch cothd
x x xdx
= - ( ) 2coth cschdx x
dx= -
Common Derivatives and Integrals
Visit http://tutorial.math.lamar.edu for a complete set of Calculus I & II notes. © 2005 Paul Dawkins
Integrals Basic Properties/Formulas/Rules
( ) ( )cf x dx c f x dx=Ú Ú , c is a constant. ( ) ( ) ( ) ( )f x g x dx f x dx g x dx± = ±Ú Ú Ú
( ) ( ) ( ) ( )b b
aaf x dx F x F b F a= = -Ú where ( ) ( )F x f x dx= Ú
( ) ( )b b
a a
cf x dx c f x dx=Ú Ú , c is a constant. ( ) ( ) ( ) ( )b b b
a a a
f x g x dx f x dx g x dx± = ±Ú Ú Ú
( ) 0a
af x dx =Ú ( ) ( )
b a
a bf x dx f x dx= -Ú Ú
( ) ( ) ( )b c b
a a c
f x dx f x dx f x dx= +Ú Ú Ú ( )b
a
c dx c b a= -Ú
If ( ) 0f x ≥ on a x b£ £ then ( ) 0b
af x dx ≥Ú
If ( ) ( )f x g x≥ on a x b£ £ then ( ) ( )b b
a a
f x dx g x dx≥Ú Ú
Common Integrals Polynomials
dx x c= +Ú k dx k x c= +Ú 11 , 11
n nx dx x c n
n
+= + ≠ -+Ú
1 lndx x cx
= +ÛÙı
1 lnx dx x c- = +Ú 11 , 1
1n n
x dx x c nn
- - += + ≠- +Ú
1 1 lndx ax b cax b a
= + ++
ÛÙı
11
1
p p p q
q q q
p
q
qx dx x c x c
p q
++= + = +
+ +Ú
Trig Functions
cos sinu du u c= +Ú sin cosu du u c= - +Ú 2sec tanu du u c= +Ú
sec tan secu u du u c= +Ú csc cot cscu udu u c= - +Ú 2csc cotu du u c= - +Ú
tan ln secu du u c= +Ú cot ln sinu du u c= +Ú
sec ln sec tanu du u u c= + +Ú ( )3 1sec sec tan ln sec tan2
u du u u u u c= + + +Ú
csc ln csc cotu du u u c= - +Ú ( )3 1csc csc cot ln csc cot2
u du u u u u c= - + - +Ú
Exponential/Logarithm Functions
u udu c= +Ú e e
ln
u
u aa du c
a= +Ú ( )ln lnu du u u u c= - +Ú
( ) ( ) ( )( )2 2sin sin cosau
aubu du a bu b bu c
a b= - +
+Úee ( )1u u
u du u c= - +Ú e e
( ) ( ) ( )( )2 2cos cos sinau
aubu du a bu b bu c
a b= + +
+Úee 1 ln ln
lndu u c
u u= +ÛÙ
ı
Common Derivatives and Integrals
Visit http://tutorial.math.lamar.edu for a complete set of Calculus I & II notes. © 2005 Paul Dawkins
Inverse Trig Functions 1
2 2
1 sin udu c
aa u
- Ê ˆ= +Á ˜Ë ¯-
ÛÙı
1 1 2sin sin 1u du u u u c- -= + - +Ú
12 2
1 1 tan udu c
a u a a
- Ê ˆ= +Á ˜+ Ë ¯ÛÙı
( )1 1 21tan tan ln 12
u du u u u c- -= - + +Ú
1
2 2
1 1 sec udu c
a au u a
- Ê ˆ= +Á ˜Ë ¯-
ÛÙı
1 1 2cos cos 1u du u u u c- -= - - +Ú
Hyperbolic Trig Functions
sinh coshu du u c= +Ú cosh sinhu du u c= +Ú 2sech tanhu du u c= +Ú
sech tanh sechu du u c= - +Ú csch coth cschu du u c= - +Ú 2csch cothu du u c= - +Ú
( )tanh ln coshu du u c= +Ú 1sech tan sinhu du u c-= +Ú
Miscellaneous
2 21 1 ln
2u a
du ca u a u a
+= +
- -ÛÙı
2 21 1 ln
2u a
du cu a a u a
-= +
- +ÛÙı
22 2 2 2 2 2ln
2 2u a
a u du a u u a u c+ = + + + + +Ú
22 2 2 2 2 2ln
2 2u a
u a du u a u u a c- = - - + - +Ú
22 2 2 2 1sin
2 2u a u
a u du a u ca
- Ê ˆ- = - + +Á ˜Ë ¯Ú
22 2 12 2 cos
2 2u a a a u
au u du au u ca
-- -Ê ˆ- = - + +Á ˜Ë ¯Ú
Standard Integration Techniques Note that all but the first one of these tend to be taught in a Calculus II class. u Substitution
Given ( )( ) ( )b
a
f g x g x dx¢Ú then the substitution ( )u g x= will convert this into the
integral, ( )( ) ( ) ( )( )
( )b g b
a g af g x g x dx f u du¢ =Ú Ú .
Integration by Parts The standard formulas for integration by parts are,
b bb
aa audv uv vdu udv uv vdu= - = -Ú Ú Ú Ú
Choose u and dv and then compute du by differentiating u and compute v by using the fact that v dv= Ú .
Common Derivatives and Integrals
Visit http://tutorial.math.lamar.edu for a complete set of Calculus I & II notes. © 2005 Paul Dawkins
Trig Substitutions If the integral contains the following root use the given substitution and formula.
2 2 2 2 2sin and cos 1 sinaa b x x
bq q q- fi = = -
2 2 2 2 2sec and tan sec 1ab x a x
bq q q- fi = = -
2 2 2 2 2tan and sec 1 tanaa b x x
bq q q+ fi = = +
Partial Fractions
If integrating ( )( )
P xdx
Q x
ÛÙı
where the degree (largest exponent) of ( )P x is smaller than the
degree of ( )Q x then factor the denominator as completely as possible and find the partial fraction decomposition of the rational expression. Integrate the partial fraction decomposition (P.F.D.). For each factor in the denominator we get term(s) in the decomposition according to the following table.
Factor in ( )Q x Term in P.F.D Factor in ( )Q x Term in P.F.D
ax b+ A
ax b+ ( )k
ax b+ ( ) ( )1 2
2k
k
AA A
ax b ax b ax b
+ + ++ + +
L
2ax bx c+ + 2
Ax B
ax bx c
++ +
( )2 k
ax bx c+ + ( )1 1
2 2
k k
k
A x BA x B
ax bx c ax bx c
+++ +
+ + + +L
Products and (some) Quotients of Trig Functions
sin cosn mx x dxÚ
1. If n is odd. Strip one sine out and convert the remaining sines to cosines using 2 2sin 1 cosx x= - , then use the substitution cosu x=
2. If m is odd. Strip one cosine out and convert the remaining cosines to sines using 2 2cos 1 sinx x= - , then use the substitution sinu x=
3. If n and m are both odd. Use either 1. or 2. 4. If n and m are both even. Use double angle formula for sine and/or half angle
formulas to reduce the integral into a form that can be integrated. tan secn m
x x dxÚ 1. If n is odd. Strip one tangent and one secant out and convert the remaining
tangents to secants using 2 2tan sec 1x x= - , then use the substitution secu x= 2. If m is even. Strip two secants out and convert the remaining secants to tangents
using 2 2sec 1 tanx x= + , then use the substitution tanu x= 3. If n is odd and m is even. Use either 1. or 2. 4. If n is even and m is odd. Each integral will be dealt with differently.
Convert Example : ( ) ( )3 36 2 2cos cos 1 sinx x x= = -
!
"
#
$!ρ,ϕ,!"
ρϕ
%ρ
%ϕ
%!
!
"
#
$
ρϕ
"ρ
ρ"ϕ
"!
ρ"ϕ
"ϕ
"ϕ
&
x = Ω cos ' Ω =
px
2+ y
2
y = Ω ' ' = arctan(y/x)
z = z z = z
uΩ
= cos 'ux
+ 'uy
u'
= ° 'ux
+ cos 'uy
uz
= uz
r = ΩuΩ
+ zuz
dr = dl
Ω
uΩ
+ dl
'
u'
+ dl
z
uz
= dΩuΩ
+ Ωd'u'
+ dzuz
dS
Ω
= dl
'
dl
z
= Ωd'dz ; dS
'
= dl
Ω
dl
z
= dΩdz ; dS
z
= dl
Ω
dl
'
= ΩdΩd'
dø = dl
Ω
dl
'
dl
z
= ΩdΩd'dz
!
"
#
$
!"sin θϕ
%!
%ϕ
%θθ
!"cos θ
!
"
#
$
ϕ
θ
!"sin θ #ϕ
!
#θ
#ϕ
!"#θ
!"sin θ #ϕ
&
#ϕ
#!
x = r µ cos ' r =
px
2+ y
2+ z
2
y = r µ ' µ = arctan(
px
2+ y
2/z)
z = r cos µ ' = arctan(y/x)
ur
= µ cos 'ux
+ µ 'uy
+ cos µuz
uµ
= µ cos 'ux
+ µ 'uy
° µuz
u'
= ° 'ux
+ cos 'uy
r = rur
dr = dl
r
ur
+ dl
µ
uµ
+ dl
'
u'
= drur
+ rdµuµ
+ r µd'u'
dS
r
= dl
µ
d
'
= r
2µdµd' ; dS
µ
= dl
r
dl
'
= r µdrd' ; dS
'
= dl
r
dl
µ
= rdrdµ
dø = dl
r
dl
µ
d
'
= r
2µdrdµd'
f = f(x, y, z) A(x, y, z) = A
x
(x, y, z)ux
+A
y
(x, y, z)uy
+
A
z
(x, y, z)uz
rf =
@f
@x
ux
+
@f
@y
uy
+
@f
@z
uz
r · A =
@A
x
@x
+
@A
y
@y
+
@A
z
@z
r£A =
√@A
z
@y
° @A
y
@z
!
ux
+
√@A
x
@z
° @A
z
@x
!
uy
+
√@A
y
@x
° @A
x
@y
!
uz
r · (rf) ¥ r2f =
@
2f
@x
2+
@
2f
@y
2+
@
2f
@z
2
f = f(Ω, ', z) A(Ω,', z) = A
Ω
(Ω,', z)uΩ
+A
'
(Ω,', z)u'
+
A
z
(Ω,', z)uz
rf =
@f
@Ω
uΩ
+
1
Ω
@f
@'
u'
+
@f
@z
uz
r · A =
1
Ω
@(ΩA
Ω
)
@Ω
+
1
Ω
@A
'
@'
+
@A
z
@z
r£A =
√1
Ω
@A
z
@'
° @A
'
@z
!
uΩ
+
√@A
Ω
@z
° @A
z
@Ω
!
u'
+
1
Ω
√@(ΩA
'
)
@Ω
° @A
Ω
@'
!
uz
r2f =
1
Ω
@
@Ω
√
Ω
@f
@Ω
!
+
1
Ω
2
@
2f
@'
2+
@
2f
@z
2
f = f(r, µ, ') A(r, µ, ') = A
r
(r, µ, ')ur
+ A
µ
(r, µ, ')uµ
+
A
'
(r, µ,')u'
rf =
@f
@r
ur
+
1
r
@f
@µ
uµ
+
1
r µ
@f
@'
u'
r · A =
1
r
2
@(r
2A
r
)
@r
+
1
r µ
@( µA
µ
)
@µ
+
1
r µ
@A
'
@'
r£A =
1
r µ
√@( µA
'
)
@µ
° @A
µ
@'
!
ur
+
1
r
√1
µ
@A
r
@'
° @(rA
'
)
@r
!
uµ
+
1
r
√@(rA
µ
)
@r
° @A
r
@µ
!
u'
r2f =
1
r
2
@
@r
√
r
2@f
@r
!
+
1
r
2µ
@
@µ
√
µ
@f
@µ
!
+
1
r
2 2µ
@
2f
@'
2
A B C
A · (B£C) = B · (C£A) = (A£B) · CA£ (B£C) = B(A · C)°C(A · B)
f = f(r) g = g(r) A = A(r) B = B(r)
r(f + g) = rf +rg
r(fg) = f(rg) + g(rf)
r · (A + B) = r · A +r · Br · (fA) = f(r · A) + A · (rf)
r · (A£B) = B · (r£A)°A£ (r£B)
r£ (A + B) = r£A +r£B
r£ (fA) = f(r£A)°A£ (rf)
r · (r£A) = 0
r£ (rf) = 0
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Di↵erential Equations Study Guide1
First Order Equations
General Form of ODE:dy
dx
= f(x, y)(1)
Initial Value Problem: y0 = f(x, y), y(x
0
) = y
0
(2)
Linear Equations
General Form: y0 + p(x)y = f(x)(3)
Integrating Factor: µ(x) = e
Rp(x)dx
(4)
=) d
dx
(µ(x)y) = µ(x)f(x)(5)
General Solution: y =
1
µ(x)
✓Zµ(x)f(x)dx+ C
◆(6)
Homeogeneous Equations
General Form: y0 = f(y/x)(7)
Substitution: y = zx(8)
=) y
0= z + xz
0(9)
The result is always separable in z:
(10)
dz
f(z)� z
=
dx
x
Bernoulli Equations
General Form: y0 + p(x)y = q(x)y
n(11)
Substitution: z = y
1�n(12)
The result is always linear in z:
(13) z
0+ (1� n)p(x)z = (1� n)q(x)
Exact Equations
General Form: M(x, y)dx+N(x, y)dy = 0(14)
Text for Exactness:@M
@y
=
@N
@x
(15)
Solution: � = C where(16)
M =
@�
@x
and N =
@�
@y
(17)
Method for Solving Exact Equations:
1. Let � =
RM(x, y)dx+ h(y)
2. Set
@�
@y
= N(x, y)
3. Simplify and solve for h(y).
4. Substitute the result for h(y) in the expression for � from step
1 and then set � = 0. This is the solution.
Alternatively:
1. Let � =
RN(x, y)dy + g(x)
2. Set
@�
@x
= M(x, y)
3. Simplify and solve for g(x).
4. Substitute the result for g(x) in the expression for � from step
1 and then set � = 0. This is the solution.
Integrating Factors
Case 1: If P (x, y) depends only on x, where
(18) P (x, y) =
My �Nx
N
=) µ(y) = e
RP (x)dx
then
(19) µ(x)M(x, y)dx+ µ(x)N(x, y)dy = 0
is exact.
Case 2: If Q(x, y) depends only on y, where
(20) Q(x, y) =
Nx �My
M
=) µ(y) = e
RQ(y)dy
Then
(21) µ(y)M(x, y)dx+ µ(y)N(x, y)dy = 0
is exact.
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Second Order Linear Equations
General Form of the Equation
General Form: a(t)y
00+ b(t)y
0+ c(t)y = g(t)(22)
Homogeneous: a(t)y
00+ b(t)y
0+ c(t) = 0(23)
Standard Form: y
00+ p(t)y
0+ q(t)y = f(t)(24)
The general solution of (22) or (24) is
(25) y = C
1
y
1
(t) + C
2
y
2
(t) + yp(t)
where y
1
(t) and y
2
(t) are linearly independent solutions of (23).
Linear Independence and The Wronskian
Two functions f(x) and g(x) are linearly dependent if there
exist numbers a and b, not both zero, such that af(x)+ bg(x) = 0
for all x. If no such numbers exist then they are linearly inde-pendent.
If y
1
and y
2
are two solutions of (23) then
Wronskian: W (t) = y
1
(t)y
02
(t)� y
01
(t)y
2
(t)(26)
Abel’s Formula: W (t) = Ce
�Rp(t)dt
(27)
and the following are all equivalent:
1. {y1
, y
2
} are linearly independent.
2. {y1
, y
2
} are a fundamental set of solutions.
3. W (y
1
, y
2
)(t
0
) 6= 0 at some point t
0
.
4. W (y
1
, y
2
)(t) 6= 0 for all t.
Initial Value Problem
(28)
8<
:
y
00+ p(t)y
0+ q(t)y = 0
y(t
0
) = y
0
y
0(t
0
) = y
1
Linear Equation: Constant Coe�cients
Homogeneous: ay
00+ by
0+ cy = 0(29)
Non-homogeneous: ay
00+ by
0+ cy = g(t)(30)
Characteristic Equation: ar
2
+ br + c = 0(31)
Quadratic Roots: r =
�b±pb
2 � 4ac
2a
(32)
The solution of (29) is given by:
Real Roots(r1
6= r
2
) : yH = C
1
e
r1t+ C
2
e
r2t(33)
Repeated(r1
= r
2
) : yH = (C
1
+ C
2
t)e
r1t(34)
Complex(r = ↵± i�) : yH = e
↵t(C
1
cos�t+ C
2
sin�t)(35)
The solution of (30) is y = yP + hH where yh is given by (33)
through (35) and yP is found by undetermined coe�cients or
reduction of order.
Heuristics for Undetermined Coe�cients(Trial and Error)
If f(t) = then guess that yP =
Pn(t) ts(A0 +A1t+ · · ·+Antn)
Pn(t)eat ts(A0 +A1t+ · · ·+Ant
n)eat
Pn(t)eatsin bt tseat[(A0 +A1t+ · · ·+Ant
n) cos bt
or Pn(t)eatcos bt +(A0 +A1t+ · · ·+Ant
n) sin bt]
Method of Reduction of Order
When solving (23), given y
1
, then y
2
can be found by solving
(36) y
1
y
02
� y
01
y
2
= Ce
�Rp(t)dt
The solution is given by
(37) y
2
= y
1
Ze
�Rp(x)dx
dx
y
1
(x)
2
Method of Variation of Parameters
If y
1
(t) and y
2
(t) are a fundamental set of solutions to (23) then
a particular solution to (24) is
(38) yP (t) = �y
1
(t)
Zy
2
(t)f(t)
W (t)
dt+ y
2
(t)
Zy
1
(t)f(t)
W (t)
dt
Cauchy-Euler Equation
ODE: ax2
y
00+ bxy
0+ cy = 0(39)
Auxilliary Equation: ar(r � 1) + br + c = 0(40)
The solutions of (39) depend on the roots of (40):
Real Roots: y = C
1
x
r1+ C
2
x
r2(41)
Repeated Root: y = C
1
x
r+ C
2
x
rlnx(42)
Complex: y = x
↵[C
1
cos(� lnx) + C
2
sin(� lnx)](43)
Series Solutions
(44) (x� x
0
)
2
y
00+ (x� x
0
)p(x)y
0+ q(x)y = 0
If x
0
is a regular point of (44) then
(45) y
1
(t) = (x� x
0
)
n1X
k=0
ak(x� xk)k
At a Regular Singular Point x
0
:
Indicial Equation: r2 + (p(0)� 1)r + q(0) = 0(46)
First Solution: y
1
= (x� x
0
)
r1
1X
k=0
ak(x� xk)k
(47)
Where r
1
is the larger real root if both roots of (46) are real or
either root if the solutions are complex.